| Preface |
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xiii | |
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Classification of defects in liquid crystals |
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1 | (16) |
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1 | (1) |
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Order and defects in a prototype model: the planar ferromagnet or the XY-model |
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2 | (2) |
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2 | (1) |
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The distorted ferromagnet |
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3 | (1) |
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4 | (1) |
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Classification of defects |
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4 | (4) |
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Testloops and winding numbers |
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4 | (1) |
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Defect equivalence and stability |
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5 | (2) |
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Defect processes and group structure |
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7 | (1) |
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Further examples of reduced order parameter spaces and fundamental groups |
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8 | (2) |
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8 | (1) |
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Two-dimensional smectics without rotations |
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9 | (1) |
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Two-dimensional periodic crystals |
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9 | (1) |
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Two-dimensional smectics with rotations |
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9 | (1) |
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Singularities in three dimensions |
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10 | (4) |
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10 | (1) |
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The Three-dimensional ferromagnet (Heisenberg-model) and point singularities |
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11 | (1) |
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Defects of three-dimensional nematics |
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11 | (1) |
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Biaxial nematics and cholesteric liquid crystals |
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12 | (1) |
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Homotopy classification of defects in three dimensions |
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13 | (1) |
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14 | (2) |
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Planar and linear topological solitons |
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14 | (1) |
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Periodic boundary conditions |
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15 | (1) |
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16 | (1) |
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Alignment tensor versus director description in nematic liquid crystals |
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17 | (20) |
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17 | (1) |
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Description of the Alignment |
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18 | (9) |
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Distribution Function and Averages |
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18 | (1) |
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19 | (8) |
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Dynamic equation for the alignment tensor |
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27 | (4) |
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27 | (1) |
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28 | (3) |
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31 | (6) |
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Visualization and s=1/2 disclination |
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31 | (1) |
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32 | (1) |
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33 | (4) |
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Liquid crystal colloidal dispersions |
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37 | (50) |
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37 | (3) |
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Colloidal Dispersions in a Nematic Solvent |
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40 | (22) |
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What is the Director Field? |
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40 | (4) |
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44 | (9) |
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Two-Particle Interactions in a Nematic Solvent |
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53 | (3) |
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Nematic Colloidal Dispersions in Complex Geometries |
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56 | (6) |
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Colloidal Dispersions above the Nematic-Isotropic Phase Transition |
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62 | (18) |
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Stability criteria for colloidal dispersions |
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62 | (2) |
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Noncharged liquid crystal colloidal dispersions at temperatures above TNI |
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64 | (10) |
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Charged spherical particles immersed in an isotropic liquid crystal |
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74 | (6) |
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80 | (7) |
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Computer simulations and defects in confined liquid crystal lattice models |
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87 | (26) |
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87 | (1) |
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Liquid Crystal Lattice Models |
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88 | (3) |
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89 | (1) |
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90 | (1) |
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Polymer Dispersed Liquid Crystals |
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91 | (13) |
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Radial Boundary Conditions (RBC) |
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92 | (12) |
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104 | (6) |
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105 | (4) |
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Schlieren textures in planar aligned cells |
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109 | (1) |
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110 | (3) |
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Molecular simulations and theory of planar interfaces and defects in nematic liquid crystals |
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113 | (28) |
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Computer simulations and theoretical approaches |
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113 | (3) |
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113 | (1) |
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114 | (1) |
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Coarse-grained descriptions |
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114 | (2) |
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Liquid crystals between parallel walls |
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116 | (3) |
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Surface anchoring coefficient |
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116 | (1) |
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Elastic boundary condition |
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117 | (2) |
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Nematic-isotropic interface |
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119 | (9) |
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Orientational order and density profiles |
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119 | (1) |
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Results at high elongation |
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120 | (2) |
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122 | (4) |
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126 | (2) |
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Disclination in cylindrical pores |
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128 | (4) |
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Defects near a colloid particle |
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132 | (5) |
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133 | (1) |
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134 | (3) |
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137 | (1) |
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138 | (3) |
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Topological defect behavior in a quenched nematic liquid crystal |
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141 | (26) |
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142 | (4) |
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146 | (2) |
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Defect-finding algorithms |
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148 | (4) |
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152 | (8) |
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152 | (2) |
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Real--space correlation function |
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154 | (2) |
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156 | (4) |
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160 | (3) |
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163 | (4) |
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Restoring forces on nematic disclinations |
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167 | (18) |
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167 | (2) |
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Restoring force and torque |
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169 | (5) |
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174 | (3) |
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176 | (1) |
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177 | (2) |
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179 | (6) |
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Challenges in the dynamics of point defects |
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185 | (16) |
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185 | (1) |
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186 | (3) |
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189 | (4) |
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Discretization of planar director fields |
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193 | (2) |
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Artefacts in numerical defect dynamics |
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195 | (6) |
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Numerical simulation of elastic anisotropy in nematic liquid crystalline polymers |
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201 | (28) |
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202 | (1) |
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203 | (3) |
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The calibration of the model |
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206 | (5) |
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Reproducing the Freedericksz transitions |
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206 | (2) |
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Topological defects in thin films |
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208 | (1) |
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Coarsening of the defects |
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209 | (2) |
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Disclinations in bulk samples |
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211 | (4) |
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212 | (2) |
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Escaped integer disclinations |
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214 | (1) |
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Texture evolution under shear flow |
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215 | (9) |
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219 | (1) |
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Interaction of wedge disclination pairs under shear flow |
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220 | (4) |
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224 | (5) |
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Computer Simulations and Fluorescence Confocal Polarizing Microscopy of Structures in Cholesteric Liquid Crystals |
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229 | (42) |
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229 | (2) |
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Mathematical basis for computer simulations of equilibrium LC structures |
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231 | (4) |
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LC structure and elastic properties |
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231 | (2) |
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233 | (1) |
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233 | (2) |
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Domain and scheme of simulations |
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235 | (1) |
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Confocal Microscopy and Fluorescence Confocal Microscopy |
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235 | (8) |
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236 | (1) |
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Fluorescence Confocal Microscopy |
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236 | (2) |
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Fluorescence Confocal Polarizing Microscopy |
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238 | (3) |
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Theoretical foundations of confocal microscopy of orientation patterns |
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241 | (2) |
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Experimental set up and materials |
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243 | (3) |
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243 | (1) |
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Liquid crystal materials and fluorescent probes |
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244 | (2) |
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246 | (14) |
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FCPM of Fredericks transition |
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246 | (1) |
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FCPM of twisted nematic cell |
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247 | (1) |
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The FCPM imaging of basic cholesteric textures |
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248 | (4) |
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Field-induced cholesteric stripes in thin cells with planar boundary conditions |
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252 | (5) |
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Cholesteric stripes in thin cells with homeotropic boundary conditions |
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257 | (3) |
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260 | (3) |
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263 | (8) |
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Defects and Undulation in Layered Liquid Crystals |
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271 | (30) |
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272 | (1) |
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Bulk Elastic and Surface Properties of Lamellar Systems |
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273 | (5) |
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Weakly distorted Smectic A phase in two dimensions |
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274 | (1) |
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Lubensky-de Gennes coarse-grained model of the cholesteric phase |
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275 | (2) |
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277 | (1) |
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278 | (8) |
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279 | (2) |
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Experimental Dislocation Profile and Non-linear Theory |
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281 | (5) |
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Layers undulations (Helfrich-Hurault instability) |
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286 | (12) |
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287 | (2) |
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Undulations Profile near the Threshold: Experiment |
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289 | (3) |
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Undulations in a Cell with a Finite Anchoring |
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292 | (2) |
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Undulations profile well above the Threshold |
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294 | (4) |
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298 | (3) |
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Liquid crystals under shear: role of defects |
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301 | (22) |
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301 | (2) |
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303 | (3) |
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303 | (1) |
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Istabilities and defects in the LE regime |
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303 | (1) |
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Instabilities and defects in the Doi regime (De ≫ 0.1) |
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304 | (1) |
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305 | (1) |
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Dislocations vs disclinations |
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306 | (3) |
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Core structure and physical properties |
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309 | (2) |
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311 | (12) |
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311 | (3) |
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Movement of isolated dislocations in a SmA phase |
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314 | (3) |
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Collective behavior of dislocations: climb of edges |
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317 | (2) |
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Collective behavior of dislocations: glide of screws |
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319 | (1) |
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A Particular case of reorganization in smectic phases: the onion texture |
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320 | (3) |
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Numerical simulation of defects in quasicrystals |
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323 | (14) |
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Crystals and quasicrystals |
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323 | (4) |
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Characteristic features of crystals and quasicrystals |
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323 | (2) |
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Structure models for quasicrystals |
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325 | (1) |
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326 | (1) |
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The cut formalism and phason-degree of freedom |
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327 | (2) |
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327 | (1) |
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Phonon and phason degree of freedom |
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328 | (1) |
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Dislocations in crystals and quasicrystals |
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329 | (3) |
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329 | (1) |
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Experimental observations |
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330 | (1) |
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Atomic interaction and numerical algorithm |
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331 | (1) |
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Dislocation motion in the two-dimensional model |
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331 | (1) |
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Dislocation motion in the three-dimensional model |
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332 | (1) |
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332 | (3) |
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335 | (1) |
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336 | (1) |
| Index |
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337 | |